Clausius–Mossotti relation
In electromagnetism, the Clausius–Mossotti relation, named for O. F. Mossotti and Rudolf Clausius, expresses the dielectric constant (relative permittivity, εr) of a material in terms of the atomic polarizability, α, of the material's constituent atoms and/or molecules, or a homogeneous mixture thereof. It is equivalent to the Lorentz–Lorenz equation, which relates the refractive index (rather than the dielectric constant) of a substance to its polarizability. It may be expressed as:
where
- is the dielectric constant of the material, which for non-magnetic materials is equal to n2, where n is the refractive index;
- ε0 is the permittivity of free space;
- N is the number density of the molecules (number per cubic meter);
- α is the molecular polarizability in SI-units [C·m2/V].
In the case that the material consists of a mixture of two or more species, the right hand side of the above equation would consist of the sum of the molecular polarizability contribution from each species, indexed by i in the following form:
In the CGS system of units the Clausius–Mossotti relation is typically rewritten to show the molecular polarizability volume which has units of volume [m3]. Confusion may arise from the practice of using the shorter name "molecular polarizability" for both and within literature intended for the respective unit system.
The Clausius–Mossotti relation assumes only an induced dipole relevant to its polarizability and is thus inapplicable for substances with a significant permanent dipole. It is applicable to gases such as N2, CO2, CH4 and H2 at sufficiently low densities and pressures. For example, the Clausius–Mossotti relation is accurate for N2 gas up to 1000 atm between 25 °C and 125 °C. Moreover, the Clausius–Mossotti relation may be applicable to substances if the applied electric field is at a sufficiently high frequencies such that any permanent dipole modes are inactive.